Atomic energy level diagrams

Thallium energy level diagram

Energy levels and transitions of neutral thallium (Tl I): the 18 strongest classified lines below 2 µm from the NIST Atomic Spectra Database and the 12 levels they connect, each line with its vacuum wavelength, frequency and, for 17 of them, the reduced dipole matrix element derived from the NIST transition rate. Measured lifetimes, transition rates, hyperfine constants and isotope shifts from the literature are included, each with its citation.

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Thallium energy level diagram with transition wavelengths and dipole matrix elements

Download: diagram (PDF) diagram (SVG) transitions (CSV) levels (CSV) source code

Key transitions of thallium

Transitionλ vac (nm)λ air (nm)ν (THz)|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Γ/2π up. (MHz)branch (%)Use
6p 2P°3/2 – 6d 2D5/2352.0234351.9228851.62644.0021.240e+08––352 nm proposed laser-cooling transition 6P3/2
6p 2P°1/2 – 7s 2S1/2377.6780377.5707793.7779411.8236.250e+0721.3646.3377.6 nm resonance line
6p 2P°3/2 – 7s 2S1/2535.1944535.0456560.15623.2667.050e+0721.3653.7535.0 nm green line
7s 2S1/2 – 8p 2P°3/2655.1663654.9854457.58221.8556.200e+061.24679.2655 nm second step of two-step spectroscopy
7s 2S1/2 – 8p 2P°1/2671.5646671.3793446.40901.0523.700e+060.864568.1671 nm second step of two-step spectroscopy
6p 2P°1/2 – 6p 2P°3/21283.25231282.9013233.6193–4.094e+006.735e-0796.71283 nm M1
7s 2S1/2 – 7p 2P°1/21301.67661301.3206230.31266.1011.710e+072.5221001301 nm second step of two-step

λ, ν from NIST level energies unless a measured frequency for this isotope is available. A: measured value or NIST. Γ/2π: natural linewidth of the upper level, 1/(2πτ).

205Tl hyperfine structure (I = 1/2)

LevelA (MHz)B (MHz)Shift of each F level from the centre of gravity (MHz)
6p 2P°1/221310.835(5)–F=0: -15983.13 F=1: +5327.71
6p 2P°3/2265.03830(10)–F=1: -331.30 F=2: +198.78
7s 2S1/212296.1(7)–F=0: -9222.07 F=1: +3074.02
7p 2P°1/22173.3(8)–F=0: -1629.97 F=1: +543.33
7p 2P°3/2311.4(3)–F=1: -389.25 F=2: +233.55
6d 2D3/2-42.9(4)–F=1: +53.62 F=2: -32.17
6d 2D5/2226.9(3)–F=2: -397.07 F=3: +283.62
8s 2S1/23870.8(14)–F=0: -2903.10 F=1: +967.70
8p 2P°1/2788.5(6)–F=0: -591.38 F=1: +197.12
8p 2P°3/2131.69(20)–F=1: -164.61 F=2: +98.77
7d 2D3/2-56.3(6)–F=1: +70.38 F=2: -42.23
7d 2D5/2180.20(20)–F=2: -315.35 F=3: +225.25

Measured A, B constants; sources in the data file.

Isotope shifts

Transitionλ vac (nm)IsotopesShift (MHz)
6p 2P°1/2 – 7s 2S1/2377.678205-2031658.3(7)
7s 2S1/2 – 8p 2P°3/2655.166203-205463.4(7)
7s 2S1/2 – 8p 2P°1/2671.565203-205450.1(8)
7s 2S1/2 – 7p 2P°1/21301.677203-205534.4(9)

Shift = ν(first isotope) − ν(second isotope).

Closed and nearly closed transitions of thallium

Transitionλ vacuum (nm)Lower levelA (s⁻¹)Leak per scattered photonPhotons before a leakWhere the leak goes
6p 2P°3/2 → 6d 2D5/2352.0234metastable1.240e+08 measured4.78 × 10−4 from theory2,0907p 2P°3/2 4.78 × 10−4*

A transition is closed when its upper level can decay only to the level it was excited from, so the atom keeps scattering photons. “closed”: among the levels NIST lists, no other level below the upper level has the opposite parity and |ΔJ| ≤ 1, so no other electric-dipole decay exists. Otherwise the leak is the sum of the branching ratios of the other decay lines of the upper level (or 1 − branching ratio where that of the line itself has been measured), and the number of photons is 1 / leak. “≥” and “≤”: at least one possible decay path has no listed rate, so the leak is a lower limit. These numbers are derived from the branching ratios, lifetimes and rates of this page, not measured as such; the tag names the weakest of the inputs, * marks theory and ≈ a model or semi-empirical calculation. Listed: lines that start on the ground level or on a metastable level and leak at most 10 %, unless more than three possible decay paths have no listed rate. Fine-structure levels only: hyperfine and Zeeman dark states and forbidden decays without a listed rate are not considered. Select a line in the diagram for the full list of its leak channels.

Listed Tl transitions below 2 µm

Lower levelUpper levelλ vacuum (nm)λ air (nm)ν (THz)Type|⟨J‖er‖J′⟩| (ea₀)A (s⁻¹)Branching (%)Source of matrix element / A
6p 2P°1/27d 2D3/2238.0306237.95801259.4701E11.082 measured4.400e+07 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°1/28s 2S1/2258.0918258.01461161.5729E10.553 NIST1.800e+07 NIST–NIST ASD (accuracy D)
6p 2P°1/26d 2D3/2276.8710276.78931082.7874E12.298 measured1.260e+08 measured78.1Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/27d 2D5/2291.9171291.83171026.9780E11.759 measured4.200e+07 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/27d 2D3/2292.2379292.15241025.8508E10.620 measured7.800e+06 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/28s 2S1/2323.0684322.9751927.9536E10.759 measured1.730e+07 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/26d 2D5/2352.0234351.9228851.6264E14.002 measured1.240e+08 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/26d 2D3/2353.0425352.9416849.1681E11.382 measured2.200e+07 measured13.6Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°1/27s 2S1/2377.6780377.5707793.7779E11.823 measured6.250e+07 measured46.3Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°3/27s 2S1/2535.1944535.0456560.1562E13.266 measured7.050e+07 measured53.7Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7s 2S1/28p 2P°3/2655.1663654.9854457.5822E11.855 measured6.200e+06 measured79.2Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7s 2S1/28p 2P°1/2671.5646671.3793446.4090E11.052 measured3.700e+06 measured68.1Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7s 2S1/27p 2P°3/21151.59611151.2809260.3278E18.453 measured2.370e+07 measured100Hunter, Commins, Roesch, Phys. Rev. A 25, 885 (1982) (abstract)
7p 2P°1/27d 2D3/21273.64201273.2936235.3820E15.475 measured7.350e+06 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6p 2P°1/26p 2P°3/21283.25231282.9013233.6193M1–4.094e+00 theory96.7Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7s 2S1/27p 2P°1/21301.67661301.3206230.3126E16.101 measured1.710e+07 measured100Hunter, Commins, Roesch, Phys. Rev. A 25, 885 (1982) (abstract)
7p 2P°3/27d 2D5/21451.82131451.4246206.4940E18.474 theory7.925e+06 theory–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7p 2P°3/27d 2D3/21459.79011459.3912205.3668E13.269 measured1.740e+06 measured–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…

Reduced dipole matrix elements follow the convention A = ω³|d|²/(3πε₀ħc³(2J′+1)), with J′ the upper level. Tags show where a number comes from: measured, NIST compilation, high-accuracy theory, this site's own Cowan-code calculation with the parameters fitted to the NIST energies (HFR fit; inputs and fit report in the repository folder cowan/; used only where nothing else gives a rate; strong lines typically within a factor 2, weak lines worse), or a model calculation.

Tl energy levels

LevelEnergy (cm⁻¹)JParityLifetimegJHyperfine A (MHz)Hyperfine B (MHz)Lifetime sourceHyperfine source
6p 2P°1/20.0001/2oddstable–21310.8––Lurio, Prodell, Phys. Rev. 101, 79 (1956) (abstract): ground-state hyperfine splitting De…
6p 2P°3/27792.7003/2odd236.3 ms theory–265.038–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…Prosnyak, Skripnikov, Phys. Rev. C 103, 034314 (2021) (arXiv:2101.01145), Sec. IV text ("…
7s 2S1/226477.5001/2even7.45 ns measured–12296.1–Norton, Gallagher, Phys. Rev. A 3, 915 (1971) (abstract; zero-field level crossing / Hanl…Chen, Fan, Chen, Lin, Chen, Shy, Liu, Phys. Rev. A 86, 052524 (2012) (arXiv:physics/07030…
7p 2P°1/234159.9001/2odd63.1 ns measured–2173.3–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…Ranjit, Kealhofer, Vukasin, Majumder, Phys. Rev. A 89, 012511 (2014) (arXiv:1310.7216), T…
7p 2P°3/235161.1003/2odd48.6 ns measured–311.4–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6d 2D3/236117.9003/2even6.2 ns measured–-42.9–Gallagher, Lurio, Phys. Rev. 136, A87 (1964) (abstract; level-crossing technique)Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
6d 2D5/236199.9005/2even––226.9––Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
8s 2S1/238745.9001/2even––3870.8––Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
8p 2P°1/241368.1001/2odd184.1 ns measured–788.5–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…Rupasinghe, Vilas, Hoenig, Wang, Majumder, arXiv:1702.06565 (2017), Table I
8p 2P°3/241740.8003/2odd127.7 ns measured–131.69–Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…Rupasinghe, Vilas, Hoenig, Wang, Majumder, arXiv:1702.06565 (2017), Table I: hyperfine sp…
7d 2D3/242011.4003/2even––-56.3––Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…
7d 2D5/242049.0005/2even––180.2––Safronova, Safronova, Johnson, Phys. Rev. A 71, 052506 (2005) (arXiv:physics/0410079), Ta…

Tl⁺ ionisation limit 49266.66 cm⁻¹ = 6.10829 eV (202.977 nm)

Sources

I(203Tl) = I(205Tl) = 1/2, so there are no B constants; for J=1/2 levels the hyperfine splitting equals A, for J=3/2 it equals 2A. rme_J_ea0 is |<J||D||J'>| in e*a0 in the Safronova convention A = 2.02613e18 S /((2J'+1) lambda^3[A]) with S = rme^2 (J' = upper level), identical to the schema convention. Entries marked compilation with "Table IV, column Z(expt)" are experimental matrix elements as collected by Kozlov, Porsev, Johnson 2001 and quoted by Safronova et al. 2005. The 7s-7p matrix elements and 7p lifetimes labelled derived come from the measured 378 nm Stark shift combined with theory (Safronova & Majumder 2013). Isotope shifts follow the SCHEMA convention nu(first)-nu(second) where the sign could be verified (378 nm: 205Tl higher); for the IR/red second-step transitions only the magnitude is certain. Extra fields beyond SCHEMA.md: hyperfine_component_frequencies_MHz, hyperfine_component_frequency_MHz, E2_M1_amplitude_ratio, PNC_E1_over_M1, A_E2_s, stark_shift_kHz_per_kVcm2, ionization_energy, mu_N. The UDel portal has no neutral Tl entry (only Tl+); neutral-atom theory comes from the Safronova-group papers.

Atoms with measured data

All elements: periodic table